Irreducible representation

A nonzero representation with no proper, nontrivial invariant subspaces.
Irreducible representation

Definition

Let (V,ρ)(V,\rho) be a finite-dimensional of a group GG over a field kk. The representation V0V\neq 0 is irreducible if its only are 00 and VV itself.

Equivalently, VV is a simple k[G]k[G]-module (compare ).

Irreducible representations are the building blocks of ones, and their characters are the .

Structural consequence (Schur)

A key fact is : for irreducible VV, GG-equivariant endomorphisms of VV are very restricted (over an algebraically closed field, they are just scalars).

Examples

  1. Cyclic groups over C\mathbb{C}: all irreducibles are 1-dimensional.
    For Cn=ggn=1C_n=\langle g\mid g^n=1\rangle and k=Ck=\mathbb{C}, every irreducible representation is

    ρj(g)=ζnjC×,j{0,1,,n1}, \rho_j(g)=\zeta_n^j\in \mathbb{C}^\times,\quad j\in\{0,1,\dots,n-1\},

    hence dim=1\dim=1. (These are precisely the complex characters of CnC_n.)

  2. Irreducibles of S3S_3 over C\mathbb{C}.
    Over C\mathbb{C}, the group S3S_3 has exactly three irreducible representations up to isomorphism:

    • the trivial 1-dimensional representation,
    • the sign 1-dimensional representation sgn\mathrm{sgn},
    • a 2-dimensional “standard” representation, realized as the action of S3S_3 on Wstd={(x1,x2,x3)C3: x1+x2+x3=0}, W_{\mathrm{std}}=\{(x_1,x_2,x_3)\in \mathbb{C}^3:\ x_1+x_2+x_3=0\}, where S3S_3 permutes coordinates of C3\mathbb{C}^3.
  3. Dependence on the field: a representation irreducible over R\mathbb{R} but reducible over C\mathbb{C}.
    Let G=C3=gG=C_3=\langle g\rangle. Consider V=R2V=\mathbb{R}^2 with

    ρ(g)=(cos(2π/3)sin(2π/3)sin(2π/3)cos(2π/3)). \rho(g)=\begin{pmatrix} \cos(2\pi/3)&-\sin(2\pi/3)\\ \sin(2\pi/3)&\cos(2\pi/3) \end{pmatrix}.

    This rotation has no real eigenvectors, hence no 11-dimensional GG-invariant subspace; therefore VV is irreducible over R\mathbb{R}. After extending scalars to C\mathbb{C}, ρ(g)\rho(g) becomes diagonalizable with eigenvalues e±2πi/3e^{\pm 2\pi i/3}, so VRCV\otimes_{\mathbb{R}}\mathbb{C} splits as a direct sum of two 11-dimensional C\mathbb{C}-representations.

See also: , .